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外延NbP和TaP外尔半金属薄膜的实现

Realization of Epitaxial NbP and TaP Weyl Semimetal Thin Films.

作者信息

Bedoya-Pinto Amilcar, Pandeya Avanindra Kumar, Liu Defa, Deniz Hakan, Chang Kai, Tan Hengxin, Han Hyeon, Jena Jagannath, Kostanovskiy Ilya, Parkin Stuart S P

机构信息

Max Planck-Institute of Microstructure Physics, Weinberg 2, 06120 Halle (Saale), Germany.

出版信息

ACS Nano. 2020 Apr 28;14(4):4405-4413. doi: 10.1021/acsnano.9b09997. Epub 2020 Feb 20.

DOI:10.1021/acsnano.9b09997
PMID:32053338
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7307967/
Abstract

Weyl semimetals (WSMs) exhibit an electronic structure governed by linear band dispersions and degenerate (Weyl) points that lead to exotic physical phenomena. While WSMs were established in bulk monopnictide compounds several years ago, the growth of thin films remains a challenge. Here, we report the bottom-up synthesis of single-crystalline NbP and TaP thin films, 9 to 70 nm thick, by means of molecular beam epitaxy. The as-grown epitaxial films feature a phosphorus-rich stoichiometry, a tensile-strained unit cell, and a homogeneous surface termination, unlike their bulk crystal counterparts. These properties result in an electronic structure governed by topological surface states as directly observed using momentum photoemission microscopy, along with a Fermi-level shift of -0.2 eV with respect to the intrinsic chemical potential. Although the Fermi energy of the as-grown samples is still far from the Weyl points, carrier mobilities close to 10 cm/(V s) have been measured at room temperature in patterned Hall-bar devices. The ability to grow thin films of Weyl semimetals that can be tailored by doping or strain, is an important step toward the fabrication of functional WSM-based devices and heterostructures.

摘要

外尔半金属(WSMs)具有由线性能带色散和简并(外尔)点所支配的电子结构,这些导致了奇异的物理现象。虽然几年前在块状单磷族化合物中就已发现了外尔半金属,但薄膜的生长仍然是一个挑战。在此,我们报告通过分子束外延自下而上合成了厚度为9至70纳米的单晶NbP和TaP薄膜。与它们的块状晶体对应物不同,生长出的外延薄膜具有富磷化学计量比、拉伸应变晶胞和均匀的表面终止。这些特性导致了一种由拓扑表面态所支配的电子结构,这是通过动量光电子显微镜直接观察到的,同时相对于本征化学势,费米能级有-0.2电子伏特的位移。尽管生长出的样品的费米能量仍远离外尔点,但在室温下,在图案化的霍尔条形器件中已测得载流子迁移率接近10平方厘米/(伏·秒)。能够生长可通过掺杂或应变进行定制的外尔半金属薄膜,是迈向制造基于外尔半金属的功能性器件和异质结构的重要一步。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/4f007817957a/nn9b09997_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/5e9b53b01fe6/nn9b09997_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/ae2bbdca47a7/nn9b09997_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/8f15217724e5/nn9b09997_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/bfbe8f8c8adc/nn9b09997_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/1710668216e6/nn9b09997_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/4f007817957a/nn9b09997_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/5e9b53b01fe6/nn9b09997_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/ae2bbdca47a7/nn9b09997_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/8f15217724e5/nn9b09997_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/bfbe8f8c8adc/nn9b09997_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/1710668216e6/nn9b09997_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fbdd/7307967/4f007817957a/nn9b09997_0006.jpg

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